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    • 1. 发明授权
    • Semiconductor device and optical module
    • 半导体器件和光模块
    • US08149891B2
    • 2012-04-03
    • US12620267
    • 2009-11-17
    • Masaki Funabashi
    • Masaki Funabashi
    • H01S5/00
    • H01S5/50G02B6/42G02B2006/12119G02B2006/12152H01S5/0202H01S5/10H01S5/101H01S5/1014H01S5/1085H01S5/227H01S5/4031H01S2301/176
    • A semiconductor laser element 10 according to the present invention comprises a waveguide 12 of a high mesa type. And then such the waveguide 12 comprises an oblique end face 17 as an emitting facet that is different from a cleaved end face 16. And hence it becomes possible to reduce a reflection factor at the end face by making of such the oblique end face 17, and it becomes possible to design a direction of an emitting beam 21, that is to be emitting from the oblique end face 17, to be independent of that for the cleaved end face 16 as well. Moreover, the emitting beam 21 is designed to be emitting as vertical to the cleaved end face 16. And then therefore in a case where an emitting beam from a semiconductor optical device is designed to be coupled with such as an optical fiber or another waveguide or the like, it is not necessary to device such as that the semiconductor laser element 10 is required to be arranged at a sub mount by being inclined to be oblique or the like.
    • 根据本发明的半导体激光元件10包括高台面型的波导管12。 然后,这样的波导12包括作为与切割端面16不同的发光面的倾斜端面17.因此,可以通过制造这样的倾斜端面17来降低端面处的反射系数, 并且可以将从倾斜端面17发射的发射光束21的方向设计成与切割端面16的方向无关。 此外,发射光束21被设计成垂直于切割的端面16发射。因此,在来自半导体光学器件的发射光束被设计为与诸如光纤或另一个波导耦合的情况下, 不需要将半导体激光元件10通过倾斜倾斜等设置在副安装台上的装置。
    • 3. 发明授权
    • Semiconductor laser device for use in a laser module
    • 用于激光模块的半导体激光器件
    • US06947463B2
    • 2005-09-20
    • US09832885
    • 2001-04-12
    • Naoki TsukijiJunji YoshidaMasaki Funabashi
    • Naoki TsukijiJunji YoshidaMasaki Funabashi
    • H01S3/094H01S3/30H01S5/024H01S5/12H01S5/227H01S5/10
    • H01S5/227H01S3/094003H01S3/302H01S5/02415H01S5/02438H01S5/0287H01S5/1212H01S5/1215H01S5/1225
    • A semiconductor laser device, module, and method for providing light suitable for providing an excitation light source for a Raman amplifier. The semiconductor laser device includes an active layer configured to radiate light, a spacer layer in contact with the active layer and a diffraction grating formed within the spacer layer, and configured to emit a light beam having a plurality of longitudinal modes within a predetermined spectral width of an oscillation wavelength spectrum of the semiconductor device. A plurality of longitudinal modes within a predetermined spectral width of an oscillation wavelength spectrum is provided by changing a wavelength interval between the longitudinal modes and/or widening the predetermined spectral width of the oscillation wavelength spectrum. The wavelength interval is set by the length of a resonator cavity within the semiconductor laser device, while the predetermined spectral width of the oscillation wavelength spectrum is set by either shortening the diffraction grating or varying a pitch of the grating elements within the diffraction grating.
    • 一种用于提供适合于为拉曼放大器提供激发光源的光的半导体激光器件,模块和方法。 半导体激光器件包括被配置为辐射光的有源层,与有源层接触的间隔层和形成在间隔层内的衍射光栅,并且被配置为发射具有预定光谱宽度内的多个纵向模的光束 的半导体器件的振荡波长谱。 通过改变纵向模式之间的波长间隔和/或加宽振荡波长光谱的预定光谱宽度来提供振荡波长谱的预定光谱宽度内的多个纵向模式。 波长间隔由半导体激光器件内的谐振器腔的长度设定,而通过缩短衍射光栅或改变衍射光栅内的光栅元件的间距来设定振荡波长光谱的预定光谱宽度。
    • 4. 发明授权
    • Semiconductor laser device having improved output power characteristics
    • 具有改善的输出功率特性的半导体激光器件
    • US06782022B2
    • 2004-08-24
    • US10189481
    • 2002-07-08
    • Masaki FunabashiRyosuke YatsuAkihiko Kasukawa
    • Masaki FunabashiRyosuke YatsuAkihiko Kasukawa
    • H01S500
    • H01S5/12
    • A semiconductor laser includes a resonant cavity with a cavity length, an active layer structure provided within the resonant cavity and configured to radiate light in an optical gain distribution having a peak wavelength, an embedding layer provided within the resonant cavity and having a refractive index, and a diffraction grating embedded within the embedding layer and having a bandgap wavelength and a refractive index, the diffraction grating configured to select an emission wavelength of the resonant cavity independently of the peak wavelength in the optical gain distribution of the active layer structure. The embedding layer and diffraction grating are configured to provide operational characteristics satisfying the relationship 0
    • 半导体激光器包括具有空腔长度的谐振腔,设置在谐振腔内的有源层结构,并且被配置为辐射具有峰值波长的光学增益分布中的光,设置在谐振腔内并具有折射率的嵌入层, 以及嵌入在所述嵌入层内并具有带隙波长和折射率的衍射光栅,所述衍射光栅被配置为在所述有源层结构的光学增益分布中独立于所述峰值波长选择所述谐振腔的发射波长。 嵌入层和衍射光栅被配置为提供满足关系0
    • 5. 发明授权
    • Semiconductor laser device
    • 半导体激光器件
    • US06661828B2
    • 2003-12-09
    • US09793881
    • 2001-02-28
    • Masaki FunabashiRyosuke YatsuAkihiko Kasukawa
    • Masaki FunabashiRyosuke YatsuAkihiko Kasukawa
    • H01S308
    • H01S5/12H01S5/2275
    • A DFB Laser of buried hetero type with a lasing wavelength of 1550 nm, having on an InP substrate a laminated structure of an InP buffer layer, an active layer, a 200-nm-thickness InP spacer layer, a 240-nm-period diffraction grating made of a 20-nm-thickness GaInAsP layer, and an InP first cladding layer in which diffraction grating is buried. The peak wavelength &lgr;max of the optical gain distribution of the active layer is approximately 1530 nm. The bandgap wavelength of the diffraction grating is approximately 1510 nm. The laminated structure is etched into mesa stripes, on both sides of which are formed p/n-separated current blocking regions. Since the diffraction grating is formed of GaInAsP having &lgr;g of approximately 1510 nm, little absorption occurs at wavelengths around the lasing wavelength 1550 nm. The absorption is coefficient with respect to the peak wavelength of the optical gain distribution of the active layer is greater than the absorption coefficient with respect to the lasing wavelength.
    • 具有1550nm的激光波长的埋入异型的DFB激光器,在InP衬底上具有InP缓冲层,有源层,200nm厚的InP间隔层,240nm周期衍射 由20nm厚度的GaInAsP层制成的光栅以及掩埋衍射光栅的InP第一包层。 有源层的光学增益分布的峰值波长lambdamax约为1530nm。 衍射光栅的带隙波长约为1510nm。 层压结构被蚀刻成台面条纹,其两侧形成p / n分离的电流阻挡区域。 由于衍射光栅由具有大约1510nm的兰德的GaInAsP形成,所以在激光波长1550nm附近的波长处几乎不发生吸收。 吸收是相对于有源层的光学增益分布的峰值波长的系数大于相对于激光波长的吸收系数。
    • 6. 发明授权
    • Gain-coupling distributed feedback type semiconductor laser device
    • 增益耦合分布式反馈型半导体激光器件
    • US06493369B2
    • 2002-12-10
    • US09865444
    • 2001-05-29
    • Masaki FunabashiAkihiko Kasukawa
    • Masaki FunabashiAkihiko Kasukawa
    • H01S500
    • H01S5/1228H01S5/0287
    • A gain-coupling distributed feedback type semiconductor laser device realizing a high light output power without causing an increase in the threshold current or a reduction in the emission efficiency, specifically a gain-coupling distributed feedback type semiconductor laser device comprised of a diffraction grating at least at part of the inside of a cavity and having a gain or loss periodically changing, a reflectance of one end surface (front facet) of the cavity being not more than 3% and the reflectance of the other end surface (rear facet) being larger than the reflectance of that one end surface and not more than 60%, such a gain-coupling distributed feedback type semiconductor laser device wherein the length of said cavity is at least 400 &mgr;m, and in particular such a gain-coupling distributed feedback type semiconductor laser device of an absorbing diffraction grating type.
    • 一种增益耦合分布式反馈型半导体激光器件,其实现高的光输出功率,而不会引起阈值电流的增加或发射效率的降低,具体地说,一种增益耦合分布反馈型半导体激光器件,其包括衍射光栅至少 在空腔的内部的一部分并且具有周期性变化的增益或损耗的情况下,空腔的一个端面(前端面)的反射率不大于3%,另一端面(后方面)的反射率较大 比所述一个端面的反射率和不大于60%的增益耦合分布反馈型半导体激光器件,其中所述腔的长度至少为400μm,特别是这样的增益耦合分布反馈型半导体 吸收衍射光栅类型的激光装置。
    • 9. 发明授权
    • Distributed feedback semiconductor laser device and laser module
    • 分布式反馈半导体激光器件和激光器模块
    • US06829277B2
    • 2004-12-07
    • US10195104
    • 2002-07-15
    • Ryosuke YatsuMasaki FunabashiAkihiko Kasukawa
    • Ryosuke YatsuMasaki FunabashiAkihiko Kasukawa
    • H01S500
    • H01S5/1228H01S5/0287
    • Disclosed is a distributed feedback semiconductor laser device having a resonator for oscillating a laser beam and a laser module which is provided with the semiconductor laser device. The semiconductor laser device comprises a diffraction grating, formed inside the resonator, for periodically changing only an extinction coefficient k or both a real refractive index n and the extinction coefficient k in a complex refractive index N expressed by N=n−ik where i is an imaginary unit. The resonator has a first facet having a first reflectance and a second facet opposite to the first facet and having a second reflectance. The first reflectance is smaller than the second reflectance and equal to or larger than 10%, preferably equal to or smaller than 20%.
    • 公开了一种具有用于振荡激光束的谐振器的分布式反馈半导体激光器件和设置有半导体激光器件的激光器模块。 半导体激光器件包括形成在谐振器内部的衍射光栅,用于周期性地仅改变由N = n-ik表示的复折射率N中的实际折射率n和实际折射率n以及消光系数k,其中i是 一个虚构的单位。 谐振器具有具有第一反射率的第一刻面和与第一小面相反并且具有第二反射率的第二小面。 第一反射率小于第二反射率,等于或大于10%,优选等于或小于20%。